{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:23AT6GEBRKSMVGYRUC6TXO4PRQ","short_pith_number":"pith:23AT6GEB","schema_version":"1.0","canonical_sha256":"d6c13f18818aa4ca9b11a0bd3bbb8f8c3e72a28022b31eeeccf2fc2295a9169a","source":{"kind":"arxiv","id":"2106.03892","version":1},"attestation_state":"computed","paper":{"title":"Ten dimensional symmetry of N=4 SYM correlators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Frank Coronado, Simon Caron-Huot","submitted_at":"2021-06-07T18:09:05Z","abstract_excerpt":"We consider four-point correlation functions of protected single-trace scalar operators in planar N = 4 supersymmetric Yang-Mills (SYM). We conjecture that all loop corrections derive from an integrand which enjoys a ten-dimensional symmetry. This symmetry combines spacetime and R-charge transformations. By considering a 10D light-like limit, we extend the correlator/amplitude duality by equating large R-charge octagons with Coulomb branch scattering amplitudes. Using results from integrability, this predicts new finite amplitudes as well as some Feynman integrals."},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2106.03892","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2021-06-07T18:09:05Z","cross_cats_sorted":[],"title_canon_sha256":"7561cf16a3d8c86b93764099dbe78079f4e2c6c9dff9d1d5f8563298b0e616af","abstract_canon_sha256":"4deb6c154999c78ccd33039785f69a8bb118fc534d773a2fd42436fa815483ed"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:13:29.998886Z","signature_b64":"sXJ+/zMpp9WlAfvGR05kG/TS7lVMwr60OMbKvvFvP5qWP84UwhXQhR9JT+jKxyperHN448b3HUEz/jl+eaf2DA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d6c13f18818aa4ca9b11a0bd3bbb8f8c3e72a28022b31eeeccf2fc2295a9169a","last_reissued_at":"2026-07-05T04:13:29.998428Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:13:29.998428Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Ten dimensional symmetry of N=4 SYM correlators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Frank Coronado, Simon Caron-Huot","submitted_at":"2021-06-07T18:09:05Z","abstract_excerpt":"We consider four-point correlation functions of protected single-trace scalar operators in planar N = 4 supersymmetric Yang-Mills (SYM). We conjecture that all loop corrections derive from an integrand which enjoys a ten-dimensional symmetry. This symmetry combines spacetime and R-charge transformations. By considering a 10D light-like limit, we extend the correlator/amplitude duality by equating large R-charge octagons with Coulomb branch scattering amplitudes. Using results from integrability, this predicts new finite amplitudes as well as some Feynman integrals."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2106.03892","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2106.03892/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"2106.03892","created_at":"2026-07-05T04:13:29.998481+00:00"},{"alias_kind":"arxiv_version","alias_value":"2106.03892v1","created_at":"2026-07-05T04:13:29.998481+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2106.03892","created_at":"2026-07-05T04:13:29.998481+00:00"},{"alias_kind":"pith_short_12","alias_value":"23AT6GEBRKSM","created_at":"2026-07-05T04:13:29.998481+00:00"},{"alias_kind":"pith_short_16","alias_value":"23AT6GEBRKSMVGYR","created_at":"2026-07-05T04:13:29.998481+00:00"},{"alias_kind":"pith_short_8","alias_value":"23AT6GEB","created_at":"2026-07-05T04:13:29.998481+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":9,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.24018","citing_title":"Null limit of large-charge correlators in planar $\\mathcal{N}=4$ Super-Yang-Mills theory","ref_index":1,"is_internal_anchor":false},{"citing_arxiv_id":"2606.30368","citing_title":"Positivity properties of observables in planar maximally supersymmetric Yang-Mills theory","ref_index":49,"is_internal_anchor":false},{"citing_arxiv_id":"2605.16034","citing_title":"Walking Sudakov: From Cusp to Octagon","ref_index":55,"is_internal_anchor":false},{"citing_arxiv_id":"2605.17056","citing_title":"Five legs @ three loops: N=4 sYM amplitude near mass-shell","ref_index":1,"is_internal_anchor":false},{"citing_arxiv_id":"2605.17057","citing_title":"Five legs @ three loops: slightly off-shell dual conformal integrals","ref_index":3,"is_internal_anchor":false},{"citing_arxiv_id":"2605.14281","citing_title":"Bootstrapping Giant Graviton Correlators","ref_index":27,"is_internal_anchor":false},{"citing_arxiv_id":"2512.21947","citing_title":"Notes on off-shell conformal integrals and correlation functions at five points","ref_index":77,"is_internal_anchor":false},{"citing_arxiv_id":"2605.14281","citing_title":"Bootstrapping Giant Graviton Correlators","ref_index":27,"is_internal_anchor":false},{"citing_arxiv_id":"2605.03887","citing_title":"Classical correlation functions at strong coupling from hexagonalization","ref_index":33,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/23AT6GEBRKSMVGYRUC6TXO4PRQ","json":"https://pith.science/pith/23AT6GEBRKSMVGYRUC6TXO4PRQ.json","graph_json":"https://pith.science/api/pith-number/23AT6GEBRKSMVGYRUC6TXO4PRQ/graph.json","events_json":"https://pith.science/api/pith-number/23AT6GEBRKSMVGYRUC6TXO4PRQ/events.json","paper":"https://pith.science/paper/23AT6GEB"},"agent_actions":{"view_html":"https://pith.science/pith/23AT6GEBRKSMVGYRUC6TXO4PRQ","download_json":"https://pith.science/pith/23AT6GEBRKSMVGYRUC6TXO4PRQ.json","view_paper":"https://pith.science/paper/23AT6GEB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2106.03892&json=true","fetch_graph":"https://pith.science/api/pith-number/23AT6GEBRKSMVGYRUC6TXO4PRQ/graph.json","fetch_events":"https://pith.science/api/pith-number/23AT6GEBRKSMVGYRUC6TXO4PRQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/23AT6GEBRKSMVGYRUC6TXO4PRQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/23AT6GEBRKSMVGYRUC6TXO4PRQ/action/storage_attestation","attest_author":"https://pith.science/pith/23AT6GEBRKSMVGYRUC6TXO4PRQ/action/author_attestation","sign_citation":"https://pith.science/pith/23AT6GEBRKSMVGYRUC6TXO4PRQ/action/citation_signature","submit_replication":"https://pith.science/pith/23AT6GEBRKSMVGYRUC6TXO4PRQ/action/replication_record"}},"created_at":"2026-07-05T04:13:29.998481+00:00","updated_at":"2026-07-05T04:13:29.998481+00:00"}